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Colin Judge: Testing structural materials in Idaho’s newest hot cell facility
Idaho National Laboratory’s newest facility—the Sample Preparation Laboratory (SPL)—sits across the road from the Hot Fuel Examination Facility (HFEF), which started operating in 1975. SPL will host the first new hot cells at INL’s Materials and Fuels Complex (MFC) in 50 years, giving INL researchers and partners new flexibility to test the structural properties of irradiated materials fresh from the Advanced Test Reactor (ATR) or from a partner’s facility.
Materials meant to withstand extreme conditions in fission or fusion power plants must be tested under similar conditions and pushed past their breaking points so performance and limitations can be understood and improved. Once irradiated, materials samples can be cut down to size in SPL and packaged for testing in other facilities at INL or other national laboratories, commercial labs, or universities. But they can also be subjected to extreme thermal or corrosive conditions and mechanical testing right in SPL, explains Colin Judge, who, as INL’s division director for nuclear materials performance, oversees SPL and other facilities at the MFC.
SPL won’t go “hot” until January 2026, but Judge spoke with NN staff writer Susan Gallier about its capabilities as his team was moving instruments into the new facility.
Ulrich Fischer
Fusion Science and Technology | Volume 13 | Number 1 | January 1988 | Pages 143-152
Technical Paper | Blanket Engineering | doi.org/10.13182/FST88-A25091
Articles are hosted by Taylor and Francis Online.
The use of beryllium as a neutron multiplier for fusion reactor blankets has been analyzed. The analysis has been performed based on designs for a helium-cooled ceramic breeder and a self-cooled liquid-metal blanket, which have both been suggested for the Next European Torus reactor. It is shown that the use of beryllium in a ceramic breeder blanket is best in a “sandwich-type” arrangement, where a beryllium block is embedded between a thin ceramic layer and the thick main breeding zone, or in a homogeneous mixture of beryllium and breeding ceramics. The sandwich-type solution needs only a minimum of beryllium inventory. Monte Carlo calculations show that heterogeneity effects in such a blanket are negligible. Therefore, the “homogeneous” solution can be achieved in a more heterogeneous arrangement like slabs of beryllium with the breeding ceramics in between. The use of beryllium also provides a benefit for liquid-metal blankets, using either LiPb or lithium metal as breeding material, since neutron multiplication and the tritium breeding ratio are enhanced in such a way that it is possible to reduce the blanket thickness considerably or to replace the inboard breeding blanket by a simple neutron reflector. It turns out that in such a blanket the use of lithium metal as breeding material is superior to that of LiPb.